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HYDRAULIC JUMP_2

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Notes on Hydraulic Jump

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  • Hydraulics Prof. B.S. Thandaveswara

    Indian Institute of Technology Madras

    28.2 Classification of Jumps

    As mentioned earlier, the supercritical flow Froude number influences the

    characteristics of the hydraulic jump. Bradley and Peterka , after extensive experimental

    investigations, have classified the hydraulic jump into five categories as shown in

    Figure 28.4.

    The hydraulic jump is the phenomenon that occurs where there is an abrupt transition

    from supercritical (inertia dominated) flow to sub critical (gravity dominated) flow. The

    most important factor that affects the hydraulic jump is the initial Froude number 1F .

    11

    VFgD

    =

    in which 1V is the longitudinal average velocity at the initial section, g is the acceleration

    due to gravity and D is the hydraulic mean depth (ratio of area of flow at free surface

    width).

    As mentioned above, it occurs in a straight prismatic horizontal channel of rectangular

    shape in which boundary friction is negligible (NHJ).

    The hydraulic jump can be classified based on initial Froude number as

    Undular ( )1 1 1 7F .= , weak ( )1 1 7 2 5F . .= , oscillating jet ( )1 2 5 4 5F . .= , steady ( )1 4 5 9 0F . .= and strong ( )1 9 0F .> .

  • Hydraulics Prof. B.S. Thandaveswara

    Indian Institute of Technology Madras

    Undular jump 1.0 < F1 < 1.7

    Weak jump 1.7 < F1 < 2.5

    Oscillating jump 2.8 < F1 < 4.8

    Steady jump 4.5 < F1 < 9.0

    Strong jump F1 > 9.0Fig. 28.4 - Classification of the Jump

  • Hydraulics Prof. B.S. Thandaveswara

    Indian Institute of Technology Madras

    Type of Jump Froude Number Remarks

    Critical flow 1F 1= Wavy surface , celerity

    c gy= Undular jump 11 < F 1 7.< Undulations on the surface Weak jump 11.7 < F 2 5.< Small rollers, No baffles.

    Oscillating Jump

    12.5 < F 4 5.<

    No periodicity. Rip rap may get damaged

    Canal drops, difficult to handle.

    Baffle blocks or appurtenances are of little value. Wave suppressors may be designed.

    Steady jump 14 5 < F 9 0. .< Position, is sensitive to

    variation of Tail Water,

    Efficiency is 45 to 70 %. Strong Jump 1F 9 0.> Efficiency is 85 %

    The jumps can also occur on horizontal bed or sloping bed. The jump can take place in

    radially diverging, radially converging, rectangular, sudden convergence or expansions

    in plan. The jump can occur in different shape of the cross section of the channel such

    as rectangular, trapezoidal, parabolic, circular channels. The jump can occur in the

    conduit either at the free surface or fully flowing downstream condition. The annular

    jump is yet another type. The jump can be either free (unsubmerged) or submerged

    condition such as in the downstream of sluice gates. The jump can be a forced one with

    the appurtenances (such as baffles, sills, chute blocks) or free (i.e. either without any

    appurtenances). Jump could be either stationary or moving (hydraulic bore).

    The jump can be in stratified flows such as warm and cold water (flowing over each

    other), air and water (classical jump) or in case of gas to gas (internal jump).

    The Important macroscopic parameters are initial depth 1y , sequent depth 2y , Initial

    mean velocity 1V , mean velocity at the end of the jump (exit velocity) 2V , length of jump

    ( )jL and the roller ( )rjL .

  • Hydraulics Prof. B.S. Thandaveswara

    Indian Institute of Technology Madras

    Classifications of Jumps

    I. Based on Froude Number

    Undular, weak, oscillating, steady and strong (See the figure - 2 above)

    II. Based on Bed Slope

    Horizontal

    ,

    Sloping

    III. plan shape of boundary

    Rectangular

    Radial Diverging Channel

    Radial Converging Channel

    Sudden Expansion

  • Hydraulics Prof. B.S. Thandaveswara

    Indian Institute of Technology Madras

    IV. Shape

    y1

    y2

    Rectangular

    T

    b

    m1

    m1

    Trapezoidal

    y1

    y2

    T

    m1

    m1

    y1

    y2

    Triangular

    T

    do

    Circular free surface flowy

    1

    doy

    1

    Circular free surface to Pressure flow

  • Hydraulics Prof. B.S. Thandaveswara

    Indian Institute of Technology Madras

    V. Fluid Status

    Water

    liquidGas

    Air

    Classical Hydraulic jump

    Gas to Gas Internal jump

    liquid (warm)1

    2 liquid (Cold)Liquid to Liquid ( 2 > 1 )

    VI. Submergence

    Sluice Gate

    1

    Hydraulicjump

    2

    3

    Rapidly varied flow with Hydraulic jump (1 and 3 subcritical flows,2 Super critical flow)

    Free Jump (Not Submerged)

    Sluice Gate

    1

    2

    3

    Rapidly varied flow with Hydraulic jump (1 and 3 subcritical flows,2 Super critical flow)

    Submerged Jump

    Tail water depth is greaterthan the sequent depth

    VII. Motion

    Stationary Jump

    Moving Jump

    Example: Hydraulic Bore

    VIII. Appurtenances

    unforced or Free

  • Hydraulics Prof. B.S. Thandaveswara

    Indian Institute of Technology Madras

    Free Jump (Unforced)(without Appurtenances)

    Forced

    Chute block Baffles or Piers or floor blocks End SillForced Jump (with Appurtenances)

  • Hydraulics Prof. B.S. Thandaveswara

    Indian Institute of Technology Madras

    Jump in gradual expanison - looking downstream

  • Hydraulics Prof. B.S. Thandaveswara

    Indian Institute of Technology Madras


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